US2432948A

US2432948A - Electric coil testing device

Info

Publication number: US2432948A
Application number: US495974A
Authority: US
Inventors: Joseph K Thompson
Original assignee: Westinghouse Electric Corp
Current assignee: Westinghouse Electric Corp
Priority date: 1943-07-24
Filing date: 1943-07-24
Publication date: 1947-12-16
Anticipated expiration: 1964-12-16

Description

Dec. 16, 1947. J, K, THOMPSQN 2,432,948

ELECTRIC CoII. TESTING DEVICE Filed July 24, 194s ATTORN EY Patented Dec. 16, 1947 ELECTRIC COIL TESTING DEVICE Joseph K. Thompson, Pittsburgh, Pa., assignor to Westinghouse Electric Corporation, East Pittsburgh, Pa.,l a corporation of Pennsylvania Application July 24, 1943, Serial N0. 495,974

7 Claims. (Cl. 175-183) My invention relates to electromagnetic devices for testing coils vin particular as to their number of turns and the presence of short circuits between the turns.

Prior to assembling any type of coil for ,the final test itis often desirable to test for the proper 'number of turns and shorts. Such a test increases in value if the assembling operation is difficult, if other windings are subsequently wound over tested sections, and if the dismantling operation is diicult as in a motor.

A known and customary method of testing coils for shorts and number of turns consists in placing the coil to be tested over a. ferromagnetic core structure with a primary or energizing winding on one portion or leg of the core structure to produce an alternating magnetic flux therein, and a standard coil of a known number of turns placed over another portion or leg. The number of turns of the test coil is determined by com'-, paring or measuring the voltage induced therein by the alternating ux in relation to the voltage induced by the same flux in the standard coll. A short in the test coil is determined by detecting the ilux distortion caused by the current owing in the shorted section.

The known devices for performing these testing methods are exacting as to the attention required for obtaining satisfactory results and involve considerable errors as regards the accuracy ofthe measuring result. These drawbacks are mainly due to the'relatively high reluctance of. the flux path and the occurrence of a considerable leakage iluX which are inevitable in such devices because of constructional requirements. That is, in order to permit the insertion and removal of the test coil, the magnetic circuit of the core structure must either be open, i. e. extend through air over. an appreciable distance, or, if a yoke is used for closing the ferromagnetic flux path, the yoke must be removable and hence involve joints or air gaps. As a result, the ilux distribution through the legs of the core structure is not uniform even if precautions are taken to keep the air gaps at a minimum. Therefore, a turn around the core leg near the energizing primary will link more flux than a turn near the open or yoke end of the core leg. Similarly, a shorted turn near the open or yoke end will produce less flux distortion than a short closer to the middle portion of the core body. Under these conditions, the measuring errors can be kept at a minimum only if the spacial distribution of the turns is identical inthe test coil and standard coil when testing for number of turns. In a coil of many turns, this is nearly impossible t achieve. Thus the lust mentioned magnetic conditions involve the exacting requirements that the standard reference coil be identical to the coil under test in its physical construction and the special location of its turns relative to one another and t-o the core body. For instance, a coil may appear to have an unsuitable number of turns while the indicated difference -is caused merely by a slight spacial displacement of the turns rela-tive j to one another. Also a slight displacement of the whole test coil, for instance by not more than the' thickness of a varnish bump, may lead to an erroneous indication. Any change in the air gaps or joints, such as caused by wear or inclusion of dirt, is also apt to affect the measuring result.

It is an object of my invention to provide coil testing devices which Vafford performing the above-mentioned testing methods while avoiding the difficulties and errors of the devices heretofore available for this purpose.

More specifically, the invention aims at reducing or eliminating the measuring errors and particular requirements due to the effect of the air gap on the flux uniformity in the known testing .devicesf Accordingly, it is an object to render the test results independent of slight displacements of the turns of a coil relative to one another and relative to the core portion or leg surrounded by them.

Another object of my invention is to eliminate or substantially reduce the disturbing effect on the test result of changes in the air gap or joint reluctance of the-testing device caused by wear, 'foreign particles or the like influences.

Still another object is to provide a testing device for the purposes described, in which a single standard or comparative coil can be used for testing specimen coils of different numbers of turns not necessarily identical or even similar to the reference coil in physical construction, l

A further object allied to those already mentioned is to render the magnetic ux in the magnetic core structure essentially uniform and largely independent of variations in the Joints or air gaps of the removable yoke member of the testing device so as to increase thereby the accuracy of measurement while reducing the amount of care and 'attention required from the operator.

In order -to achieve these objects and advantages in accordance with my invention, the testing device is designed so that only the standard coil and the specimen coil are arranged on the main core structure while the energizing primary coil for producing the alternating magnetic flux is disposed on the movable or removable yokemember of the structure. When in operation, the ux produced by the primary has to pass through the joints or air gaps before it enters the core body proper which has a uniformly low reluctance path and links itself with the standard and specimen coil placed on the core body.

According to another and subsidiary aspect, the invention provides a testing device designed as just mentioned in which a subdivided and tapped standard coillor a plurality of selective standard coils are used so that the coils to be tested may have different numbers of turns without requiring more than the setting of a selective contactor or the like adjusting member for rendering the device applicable to the particular test coil under observation.

In another aspect, the invention provides a variable and selectively adjustable circuit member outside the testing device proper but arranged in the appertaining measuring circuit for adjusting the measuring range to a specimen under test; while employing eluniversal standard coil for comparison with specimen coils of different numbers of turns.

The above-mentioned and other objects and features of the invention will be apparent from the following description of several embodiments taken in conjunction with the appertaining drawing in which:

Figure 1 represents a diagram of a coil testing device according to the invention in connection with an electric energizing circuit and a measuring circuit for indicating the test result;

Fig 2 illustrates diagrammatically another embodiment of a testing device also in accordance with this invention, and

Fig. 3 represents a coil testing device similar to the one shown in Fig. 1 but provided with a different measuring circuit.

While the above-mentioned figures refer to the indication of the number of turns of a coil to be tested, Fig. 4 shows diagrammatically a similar device and its application to a test for determining the presence of short circuits between the turns of a coil. y

Figs. 5 through 9 are explanatory views and serve to elucidate the operation of a testing device designed in accordance with the principles of my invention by comparing it with testing devices similar to those of the prior art and not in compliance with the requirements of .the invention.

More particularly, Fig'. 5 shows the flux distribution in a magnetic structure as heretofore used for testing purposes of the kind here in point having a high reluctance path for the flux enclosed by coils; while Fig. 6 represents a flux diagram relating to the same type of core structure.

Fig. 'l shows another magnetic structure of the type heretofore in use, the diagram of Fig. 6 being in substance also applicable to the latter type of devices.

In comparison, Fig. 8 shows the flux distribution in a magnetic structure embodying the principles of this invention and Fig. 9 an appertaining flux diagram.

Fig. l0 represents a further embodiment of a testing device according to the invention.

Referring to Fig. l, numeral I0| denotes a substantially U-shaped laminated core body of ferromagnetic material, for instance alloy steel of high magnetic permeability and negligible magnetic remanence. The oor@ body has two legs |02 and |03 extending in parallel to each other. The outer ends of these legs are bridged by a yoke |04 which is formed as a separate body and consists preferably also of a laminated structure of a highly permeable material of the kind just mentioned. The yoke |04 is removable from the core body |0I; However, it may be linked at one end to leg |02 of the core body I0| so that the other end can be turned away or up from the respective leg. Another way of construction is to provide a. slidable engagement between the yoke |04 and the legs |02 and |03, so that the yoke can be moved away from leg |02 to permit inserting and exchanging the specimen coil mentioned hereinafter.

The removable yoke |04 is provided with a primary coil III which serves to energize the electromagnetic test system. The terminals |I2 and ||3 of the primary coii I|| are connected to a -suitable source |00 of alternating current. When the yoke is in proper position and the primary coil energized, a magnetic flux is passed through the magnetic structure which offers the flux an essentially closed ferromagnetic path interrupted by more reluctant material only at the joints or air gaps between the legs and the yoke |04.

A standard coil I|4 of a known number of turns is arranged on leg |02. The specimen coil 1 to be tested is placed over leg-|03. When performing the test, the terminals ||5 and IIS of the standard coil ||4 are connected by leads |05 and |06 with the corresponding terminals IIB and I|9 of the specimen coil An indicating or recording measuring instrument |01 is inserted into one of the connecting leads and is provided with a scale |08 or other means for lndicating any difference between the number of turns of the specimen coil ||1 and standard reference coil H4.

It will be seen from Fig. l that the two legs |02 and |03 of core body |0| are series arranged to each other in magnetic respect so that the same magnetic flux, generated by the primary winding Il I, passes uniformly through both coils ||4 and |I'|. Consequently, if the coils have the samenumber of turns, the same voltage is produced in each coil. The two secondary voltages thus obtained oppose and balance each other in the measuring circuit. Hence the instrument |01 will indicate zero on scale |08. However, if the specimen coil II'I has more or fewer turns than the standard coil II4, its secondary voltage will differ from that of the standard coil and will cause an unbalance current to flow through the measuring circuit. As a result the instrument |01 will deflect the extent of deflection being a measure of the difference in the number of turns.

While the measuring method involved in the test just described is essentially similar to the customary testing methods referred to .in an earlier place of this specification, it will also be seen that the device according to the invention functions more advantageously than the known testing devices as regards the eiect of air ga'ps and high reluctance points between the yoke |04 and the legs |02 and |03 of the core body. Due to the fact that the primary winding I l is arranged on the yoke |04 while the standard coil and specimen coil are both placed on the core body proper, any variation in the gap reluctance will show up only as a variation in magnetizing current of coil I|| and hence will have no eect on the test result. The leakage ilux is limited to the immediate neighborhood of the gap, and the sans tlux portion actually introduced into the main core structure will have a continuous' low reluctance path over the entire iron structure linking the standard and test coils.

Because of the uniform iiux distribution in the main core body, all coils having the same number oi turns will give the same indication regardless of their location along the ilux path. It is not necessary that the spacial distribution be the same or that the coils be located on the test leg with any geometrical precision. Hence, a tapped coil having a proper number of turns can be used to test any coil of any shape having the same number of turns.

A testing arrangement of the latter type is illustrated in Fig. 2. According to this figure, a core body 20| with two

parallel legs

202 and 203 is provided with a yoke 204 which is removable from the core body to a suillcient extent to permit placing the specimen coil 2 I 1 over one of the legs. The core body 20| in Fig. 2 is shown as partly broken away in order to show some of the laminations denoted by I, 2, 3 and 4. 'I'he reference winding arranged on leg 202 of the magnetic structure comprises, for instance, three groups of turns marked 2|4, 224, and 234. Each oi' these groups is tapped and connected with corresponding groups of contacts denoted by 244, 254 and 264, respectively. Each group cooperates with a

slide contact

214, 284, 294, respectively. In this manner, a plurality of contact devices areformed which permit a selective adjustment of the reference winding as to the number of turns inserted between the terminals 2 I5 and 2I6. The group of turns denoted by 2|4 has many windings, the group 224 has a smaller number of turns while the smallest number of turns is allotted to group 234. The gradation of the groups of turns and appertaining contacts is preferably chosen in accordance with a decimal system or a geometric progression so as to permit varying the eifective number oi' turns over a 'relatively large range of adjustment. The terminals 2I5 and 2I6 of the reference winding and the terminals 2I8 and 2|! of the specimen coil 2I1 are connected with a detector circuit and a measuring, indicatingor recording instrument which may be similar to known" devices because of the above mentioned difiiculties encountered therein, the uniformity of the magnetic flux over virtually the entire length of the core body in devices according 4to the in vention makes it possible to employ this arrangement to advantage, and hence permits rendering one and the same testing device more versatile than the testing means heretofore available.

Since a tapped standard or reference coil may be used, it is also possible to so arrange the' testcircuit to indicate an excess or deiiciency in the number of turns so that the coil to be tested can be compared to sections of the reference having the minimum and maximum number of allowable turns. This test procedure makes it unnecessary to actually determine the number of turns in the test coil; that is such a procedure is similar to the "go and no go tests applied when testing mechanical fixtures by gauges which do not actually determine the dimensions .of the tested specimen.

Since it is often necessary to test coils which have relatively few turns, the test circuit must 8 have sumcient sensitivity to detect adifferenoc of one or a few turns between the standard and test coils. For this reason, the indicating instrument is preferably used as a null voltage or current indicator. This null indicator may be a galvanometer, or a circuit combination such as a vacuum tube voltmeter. oscilloscope lor the like tion per one-turn difference will vary inversely with the number of turns in the coil undertest. In accordance with this aspect, the basic sensitivity of one-turn diil'erence is reduced in proportion to the required number of turns in the test coil. For example, one turn represents 2% difference in a coil of 50 turns, 1% in a coil of 100 turns, or 0.1% in coils of 1000 turns and approaches a wholly negligible value for coils of more turns.

For instance, if the turn difference allowed is set at 2%, I propose to diminish the sensitivity of thev testing apparatus to 2% oi' the desired number of turns in the test coil. This wouldbe 1 turn for a 50turn coil, 2 turns for a 10U-turn coil, 20 turns for a 1000-turn coil, and so forth. When performing this method, a sensitive voltage detector, such as an A. C. galvanometer or a rectier system with a D'Arsonval movement or a vacuum tube voltmeter, oscilloscope, or wattmeter separately excited or the like apparatus, may be used in order to keep the test current at a minimum.

An embodiment of the just mentioned type is represented by Fig. 3. According to this figure, the magnetic core body 30| has a standard coil 3|4 arranged on its leg 302 and a specimen coil 3|1 arranged on leg 303. As in the proceeding embodiments, the two legs are magnetically bridged by a magnetizable yoke 304 which carries the primary winding 3| I whose terminals 3I2 and 3I3 are to be connected with an alternatingcurrent source. Terminals 3|5 and 3|6 ofy the standard coil 3|4 are connected with terminals 3| 3 and 3I9 of the removable specimen coil 3I1 by a measuring circuit which contains a sensitive voltage-detector at 301 and is also provided with a tapped impedance 321. The taps 331 form part of a selective switch arrangement, the 'movable switch contact being designated by 341. The impedance 321, or rather the magnitude of the impedance lying between each pair of taps, isso graduated along the path of motion of the con tact member 341 that the rate of change of the resistance increases in the direction from th'e top to the bottom of the path of motion. Hence, relatively few turns or low impedance magnitudes are effective between the pairs of contacts at the top of the arrangement whilethe number of turns or the magnitude of the impedance is higher between the contacts of a pair closer to the bottom of the arrangement. By adjusting the movable contact 341, the sensitivity of thev arrangement can be adapted to the particular specimen under observation.

If the switch 341 leaves the major portion of the impedance in series with the indicating means a large turn diiierence must be present to give indication. This would be the proper adjustment for testing a coil of many turns.

For a test coil of few turns, the'impedance is more or less shunted out by adjusting the switch 341, thus increasing the over all sensitivity and enabling the detector to indicate as little as a one-turn dierence.

The above-mentioned impedance should preferably be proportional to the'voltage produced per turn on the test coil and the indicator so marked that each position of switch 341 corresponds to a proper range of turns for the coil to be tested.

Furthermore, if a xed percentage difference is to be maintained between the standard and test coils, the indicator can be made to operate with an approximate half-scale deilection. More or less turns would thus give a reading in a more accurate scale position and no deiiection would indicate an open coil with no separate test necessary forl this important determination,

While the adjusting impedance is shown as a tapped series resistor in Fig.- 3, it will be understood that other types of impedance devices and other circuit arrangements may be used instead for achieving the above-mentioned measuring function.

Fig. 4 shows a testing device similar to those of Figs. l,y 2 and 3 but applied for testing a specimen coil as to the presence of short circuits between the turns of the coil. The core body 40| carries identical balancing coils 4I4 and 4 I 5 whose terminals are connected in bucking connection with a meter 401 or the like measuring device or circuit for determining the absence of secondary voltage or current effective across the balancing coils when the primary winding 4|| disposed on the yoke 404 is energized by connecting its terminals 4 I 2 and 4|3 to an alternating current source. The coil to be tested is denoted by 4|1. It is placed over one of the legs of the core body with its terminals 4|8 and 4I9 left open. Ii' the specimen coil is free of shorts, the secondary balance indicated by 401 is not appreciably varied by placing the coil 4|1 over the legs. If, however, a short is present, the current ilowing i'n the 'shorted turns produces a countermagnetomotive force which forces a portion of the iiux to assume the path diagrammatically shown in Fig. 4 by a` broken line. As a result, one portion of the balancing coil 4|4 will link less magnetic flux than the other portion. Consequently, the indicating instrument 401 will be aiected by an imbalance current or Voltage and produce a corresponding indication. It will be obvious from the foregoing explanation that the advantages of the invention are also effective in a testing arrangement of the latter type because the position of the test coill relative to the core'leg has little eilect on the indicator means.

The function and advantages of a device according to the invention will be more fully understood from the explanatory diagrams of Figs. 5 through 9. I

Fig. 5 represents a magnetic structure for testing purposes of the kind here dealt with, the structure being designed similar to those heretofore known, and hence not in accordance with the present invention. The primary winding 5|| is placed on the core body 50| proper. 5|! and 5|3 denote the terminals of the primary coil. They `are to be`eonnected to an alternating-current source. 5|4 is the required unique reference coil :with terminals -5|5 and SIS, and 5|1 is the exchangeable specimen coil with terminals 5l8 and SIS.. The terminals of coils .5|4' and 5I1 which must be identical are to be connected in a measuring circuit similar to those employed in connection with the present invention. Due to the high reluctance of the joints and high leakage because the magnetic ilux is, not generated within the yoke member 004. the A:magnetic flux through the system has the approximate distribution indicated schematically by the dotted lines. The flux has its greatest density within the primary winding 5| I and shows increasing leakage towards the gaps or joints between the ends of the legs and the adjoining yoke 504.

The ilux density along one grammatically shown in Fig. 6. In this diagram the abscissa represents ilux densities, and the ordinate the distance from the base portion of the core structure along the leg, the total distance between the zero point O and point D being indicated in Fig. 5 by a line also marked O-D. The flux density represented by l,curve l in Fig. 6 is a minimum'at the air gap or joint and increases gradually to a maximum which appears close to the primary winding,

Substantially the same flux distribution obtains in a testing device of the type shown in Fig. 7. In the latter device, a W-'shaped core body 10| is employed with three parallel legs 102, 103 and4 109. The primary windings 1|I are placed on the center leg 109 while the two other legs are occupied by the reference coil 1I4 and the removable specimen coil 1|1 respectively whichl must be identical. A yoke 104 is provided to bridge the three legs 102, 103 and 109. Thev similarity of flux distribution in either 'leg 102 or 103 to the one discussed with reference to Fig. 5 is due to the facts that the energizing coil 1|| is disposed on the core body proper 10|, and the flux is forced through the high reluctance of the joints with the yoke member 104.

In contrast to the arrangements just discussed, Fig. 8' shows schematically the flux distribution in the magnetic structure of a device according to the invention. Since the iiux is.generated by the primary coil 0I I within the yoke member 004, the leakage ilux is substantially limited to the immediate neighborhoodof the gap or joints. Consequently, as stated in the foregoing, the ux is substantially uniform along the entire magnetic length of the core body 00| proper. This is apparent from the diagram of Fig. 9 showing the flux density in one of the legs with reference to the distance from the base portion of the core body, the total distance O'D' being indicated in Fig. 8 by a line also marked O-D'. According to'Fig, 9 the iiux density is at a maximum (Max) near the 'yoke and drops in the leg portion close to the yoke to a minimum value (Min'). This value is maintained over the predominant portion of the length of the leg and is also effective in the base portion of the core body extending at a right angle to the leg.

The embodiment shown in Fig. 10 diifers from those previously described in having the leg 002 and bottom portion of the core body 60| designed with a larger cross section than the leg 600 carrying the specimen coil SI1. This permits keeping the reluctance of the iiux path at a minimum for obtaining a uniform ux and low leakage without exceeding the maximum dimensions of the core required within the specimen coil. 004 denotes the yoke member, BII the magnetizing primary, and 6|4 the reference coil.

While I have illustrated a limited number of embodiments, it will be obvious to those skilled in the art that many changes as to the shape 9 and arrangement of the magnetic structure and coils are possible without departing from the principles and advantages of this invention.

For instance, one or both of ,theA standard and specimen coils may also be arranged on the base portion of the core body rather than on the legs. Furthermore, the magnetizlng coil, or this coll and the yoke member may be replaced by a permanentl magnet for certain types of application.

It will also be apparent -that a number of dif-v ferent measuring circuits may be connected to the coils of the device in order to indicate the number of turns or the occurrence of shorts as set forth in this specification. Therefore, I intend the above described embodiments to be considered as illustrative but not in a. limiting sense as to the scope of my invention.

I claim as my invention:

1. An electric coil testing device comprising a substantially U-shaped laminated magnetizable core having leg portions arranged in magnetic series connection, a substantially straight ferromagnetic yoke `for bridging. said core so as to establish an essentially closed magnetic circuit through said core, an energizing primary winding arranged on said yoke, said yoke and said primary winding being removable from said core, a reference coil arranged on one of said leg portions, another of said leg portions being designed for removably accommodating a coil to be tested, 2. An electric device for the testing of coils, comprising a ferromagnetic and substantially U- shaped core body, a removable ferromagnetic yoke for bridging said body so as to provide an essentially closed ferromagnetic circuit when placed against said body, an energizing primary winding arranged on said removable yoke, a reference coil arranged on said core body, said core body having a free portion designed for removably accommodating a coil to be tested so that, during a test, the coil to be tested is traversed by a magnetic ilux produced by said primary winding and of fixed proportion to the flux passing through said reference coil. 3. An electric device for the testing of coils, comprising a magnetizable and substantially LJ- shaped core body having two legs extending substantially in parallel to each other, a reference coil arranged on one of said legs, said other leg being designed for removably accommodating a coil to be tested, a magnetizable yoke for bridging said legs so as to establish together with said core body an essentially closed magnetic circuit, said yoke being movable relative to said core body so as to permit placingia coil to be tested on said other leg, and a primary energizing winding disposed on said movable yoke for passing magnetic vilux through said legs.

4. An electrical coil testing device comprising a substantially U-shaped ferromagnetic core body, a removable ferromagnetic yoke for bridging said body in order to provide an essentially closed ferromagnetic circuit when placed against said body, an energizing primary winding arranged on said yoke so as to be removable together with said yoke, a standard winding arranged on said core body, said winding having taps so as to be subdivided into a number of groups of turns, said groups being diiferent from one another as to the number of included turns, selective contact means connected with said taps for changing the total number of effective turns of said standard winding in accordance with the diierence in the turn number of said groups, said core body being dethat, during a test, the coil to be tested is traversed by a magnetic flux produced by said primary Winding and of fixed proportion to the iiux passing through said standard winding.

5. An electrical coil testing device comprising a substantiallyU-shaped ferromagnetic core body, a removable ferromagnetic yoke for bridging said body in order to provide an essentially closed ferromagnetic circuit when placed against said body, an energizing primary winding arranged on said yoke so as to be removable together with said yoke, a standard winding arranged on said core body, said winding having taps so as to be subdivided into a number of groups of turns, said groups being different from one another as to the number of included turns in accordance with a decimal gradation, selective contact means connected with said taps for changing the total number of effective turns of said standard winding, said core body being designed for accommodating a coil to be tested so that, during a test, the coil to be tested is traversed by a magnetic ilux produced by said'primary winding and of iixed proportion to the flux passing through said standard winding.l

6. An electric coil testing device comprising a substantially U-shaped magnetizable core body having two series arranged portions, a standard coil arranged on one of said portions, said other core portion being designed for accommodating a coil to be tested, a magnetizable yoke for bridging said core body in order to establish an essentially closed magnetic circuit, said yoke being removable from said core body to permit placing the coil to be tested on said other core portion, a primary energizing winding disposed on said removable yoke for passing magnetic flux through said portions, a secondary circuit for connecting said standard coil with the coil to be tested, said circuit containing a measuring instrument and an adjustable impedance member for varying the sensitivity of said circuit.

7. An electrical coil testing device comprising a substantially U-shaped ferromagnetic core body, a removableyoke structure for bridging said body having magnetizing means for passing a magnetic flux through said body and forming together with said body an essentially closed ferromagnetic circuit when placed against said body, a reference coil on said core body, said core body being designed for accommodating a coil to be tested sothat, duringa test, the coil to be tested is traversed by a magnetic ux of fixed proportion to that passing through said reference coil.

JOSEPH K. THOMPSON.

REFERENCES CITED The following references are-of record in the ille of this patent:

UNITED STATES PATENTS OTHER REFERENCES Isaacson, Radio News, May 1931, pp. 989, 1025 and 1027.